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Principles of Fluorescence Spectroscopy

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178 FREQUENCY-DOMAIN LIFETIME MEASUREMENTS<br />

Figure 5.26. Frequency-domain measurements <strong>of</strong> the intensity decay<br />

<strong>of</strong> NADH up to 2-GHz. From [3].<br />

a vasoconstrictor. Vasopressin is a cyclic polypeptide that<br />

contains 9 amino acids including a single tyrosine residue<br />

at position 2. Oxytocin has a similar structure, but has a distinct<br />

physiological activity <strong>of</strong> stimulating smooth muscle<br />

contraction. Hence there have been many efforts to use the<br />

tyrosine emission to learn about the solution conformation<br />

<strong>of</strong> these peptide hormones. The frequency-domain data for<br />

vasopressin reveal a complex intensity decay (Figure<br />

5.27). 114 The decay is not even closely approximated by the<br />

single exponential model (dashed). Fitting the data requires<br />

three decay times <strong>of</strong> 0.17, 0.75, and 1.60 ns. These multiple<br />

decay times could probably not be recovered if the data<br />

were limited to 200 MHz.<br />

MCP PMTs are moderately expensive, and their use in<br />

FD measurements requires special circuits for cross-correlation.<br />

However, the advantages <strong>of</strong> high-frequency FD data<br />

may become available without the use <strong>of</strong> MCP PMTs.<br />

Examination <strong>of</strong> Figures 5.26 and 5.27 indicates that considerable<br />

data can be obtained if the data were available to just<br />

1 GHz. This frequency limit can probably be reached with<br />

the new compact PMTs, which show short transit time<br />

spreads (Table 4.1). A dynode PMT (H5023) has already<br />

been used up to 1 GHz. 115 It seems likely that a compact<br />

PMT such as the R74000 will be useful up to 900 MHz.<br />

Laser diodes with 30-ps pulse widths will provide useful<br />

harmonics up to 40 GHz.<br />

Figure 5.27. Phase and modulation data for the vasopressin tyrosine<br />

fluorescence intensity decay. The dashed line is the best single-exponential<br />

fit, and the solid line is the best three-exponential fit. From<br />

[114].<br />

In the near future gigahertz FD instruments will be<br />

available based on pulsed-laser diodes and compact PMTs.<br />

5.7. ANALYSIS OF FREQUENCY-DOMAIN DATA<br />

Frequency-domain data is <strong>of</strong>ten analyzed in terms <strong>of</strong> the<br />

multi-exponential model. As described in Chapter 4, the<br />

amplitudes (α i ) and decay times (τ i ) are usually strongly<br />

correlated, so that there can be considerable uncertainty in<br />

the values <strong>of</strong> the recovered parameters. In this section we<br />

describe examples that show correlation between the<br />

parameter values.<br />

5.7.1. Resolution <strong>of</strong> Two Widely Spaced Lifetimes<br />

The analysis <strong>of</strong> frequency-domain data can be illustrated<br />

using a mixture <strong>of</strong> p-terphenyl and indole. This same mixture<br />

was used in Chapter 4 for TCSPC data (Figures 4.46–<br />

4.49). The same 292-nm excitation and 330-nm emission<br />

wavelengths were used for the frequency-domain measurements<br />

as for the time-domain measurements. The decay<br />

times <strong>of</strong> the individual fluorophores are 0.93 and 3.58 ns for<br />

p-terphenyl and indole, respectively. For this mixture the<br />

decay times are spaced 3.8-fold, making this a moderately

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